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Our calculations show that reasonable coupling efficiencies can be realized. , a lower than expected output voltage results). Thus we performed calculations to determine coupling coefficients of various geometries to understand this effkct. -29- V. REFERENCES [1] G. J. Caporaso, “Induction Linacs and pulsed Power:’ in Proceedings 1994 Joint Topical Course, Maui, HI (1994). [2] J. Elizondo and A. Rodriguez, ‘Wovel High Voltage Surfitce Flashover Insulator Technology,” in Proceedhgs of the 1992, 15th International Symposium on Discharges and Electrical Insulation in Vacuum Ber@ Germany (1992).

Sampayaq et. , “High Gradient Insulator Technology for the Dielectric Wall Accelerator,” in Proceedings of the 1995 Particle Accelerator Conference, Dallas,TX(1995). [4] S. Sampay~ et. , “High Pefiorrnance Insulator Structures for Accelerator Applications: Lawrence Livermore National Laborato~ Report, UCRL-53868-% (1996). [5] S. C. Zhang, Department of Ceramic Engineering, University of Missouri, Roll% MO, pri- vate communication. [6] S. Sampayrq et. , ‘llptkdly Induced Surface Flashover Switching for the Dielectric Wall Accelerator; in Proceedings of the 1995 Particle Accelerator Conference, Dallas, TX (1995).

The electromagnetic characteristics of the HGI are due to perturbing the geometry of the resonant cavity. Carefil incorporation of HGI’s into an induction cell design should always lead to a much lower impedance than that of a conventional solid insulator. Further, as the higher voltage hold off of the HGI allow for narrower gaps and the transverse impedance scales directly with gap widt~ an additional faaor of two reduction is expected. Second, we performed circuit modeling to understand energy coupling to dynamic loads by the Asymmetric Blurnlein.

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Advanced Accelerator Theory Development


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